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arXiv 1102.3000cond-mat.mes-hallcond-mat.supr-con
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量子线中的强耦合拓扑约瑟夫森效应

Strong-coupling topological Josephson effect in quantum wires

Flavio S. Nogueira, Ilya Eremin

摘要:

我们研究了具有两个晶格量子线的装置的约瑟夫森效应,该装置在隧道结处具有马约拉纳零能边界模。在弱耦合情况下,精确解再现了包含$\sim \pm\cos(ϕ/2)$贡献的能量相对于成对Majorana费米子隧穿的微扰结果。随着隧道幅度$g$相对于跳跃幅度$w$的增长,能级之间的间隙逐渐减小,直到其在临界值$g_c=\sqrt{2}w$处完全闭合。在这一点上,约瑟夫森能量具有主值$E_{mσ}=2σ\sqrt{2}w\cos[ϕ/6+2π(m-1)/3]$,其中$m=-1,0,1$和$σ=\pm 1$,这不是微扰理论的结果。它代表了一个透明的制度,其中三个Bogoliubov状态合并,导致额外的拓扑非平凡的基态与奇数马约拉纳费米子在每根线的末端简并。在本征态宇称固定的情况下,我们也得到了精确的隧道电流。约瑟夫森电流显示了拓扑约瑟夫森效应所期望的特征$4π$周期性。我们讨论了与闭合的能级之间的能隙相关的电流的附加特征。

英文摘要:

We investigate the Josephson effect for a setup with two lattice quantum wires featuring Majorana zero energy boundary modes at the tunnel junction. In the weak-coupling, the exact solution reproduces the perturbative result for the energy containing a contribution $\sim \pm\cos(ϕ/2)$ relative to the tunneling of paired Majorana fermions. As the tunnel amplitude $g$ grows relative to the hopping amplitude $w$, the gap between the energy levels gradually diminishes until it closes completely at the critical value $g_c=\sqrt{2}w$. At this point the Josephson energies have the principal values $E_{mσ}=2σ\sqrt{2}w\cos[ϕ/6+2π(m-1)/3]$, where $m=-1,0,1$ and $σ=\pm 1$, a result not following from perturbation theory. It represents a transparent regime where three Bogoliubov states merge, leading to additional degeneracies of the topologically nontrivial ground state with odd number of Majorana fermions at the end of each wire. We also obtain the exact tunnel currents for a fixed parity of the eigenstates. The Josephson current shows the characteristic $4π$ periodicity expected for a topological Josephson effect. We discuss the additional features of the current associated with a closure of the energy gap between the energy levels.

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